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Volumn 85, Issue 18, 2000, Pages 3938-3941

Resonances, instabilities, and structure selection of driven Josephson lattice in layered superconductors

Author keywords

[No Author keywords available]

Indexed keywords

COMPUTER SIMULATION; CURRENT VOLTAGE CHARACTERISTICS; ELECTRIC FIELD EFFECTS; LATTICE CONSTANTS; MAGNETIC FIELD EFFECTS; MAXWELL EQUATIONS; NUMERICAL ANALYSIS; OXIDE SUPERCONDUCTORS; PLASMA WAVES; VELOCITY;

EID: 0034292676     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevLett.85.3938     Document Type: Article
Times cited : (52)

References (24)
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    • Kleiner, R.1
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    • We do not consider resonances related to the finite-size effect (Fiske resonances). The Fiske resonant frequencies for layered superconductors have been classified by R. Kleiner, Phys. Rev. B 50, 6919 (1994) and detected experimentally by A. Irie, Y. Hirai, and G. Oya, Appl. Phys. Lett. 72, 2159 (1998).
    • (1994) Phys. Rev. B , vol.50 , pp. 6919
    • Kleiner, R.1
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    • 0032045926 scopus 로고    scopus 로고
    • We do not consider resonances related to the finite-size effect (Fiske resonances). The Fiske resonant frequencies for layered superconductors have been classified by R. Kleiner, Phys. Rev. B 50, 6919 (1994) and detected experimentally by A. Irie, Y. Hirai, and G. Oya, Appl. Phys. Lett. 72, 2159 (1998).
    • (1998) Appl. Phys. Lett. , vol.72 , pp. 2159
    • Irie, A.1    Hirai, Y.2    Oya, G.3
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    • S. Sakai, P. Bodin, and N. F. Pedersen, J. Appl. Phys. B 73, 2411 (1993); L.N. Bulaevskii et al., Phys. Rev. B 50, 12 831 (1994).
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    • For a convective instability a localized perturbation grows exponentially at some moving frame and decays at fixed point. For an absolute instability the perturbation grows at any fixed point, see, e.g., E. M. Lifshits and L. P. Pitaevskii, Physical Kinetics (Pergamon Press, Oxford, New York, 1981).
    • (1981) Physical Kinetics
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  • 23
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    • The opposite case describes the scattering of the incoming wave generated far away from the boundary with the wave vector given by an external source (or opposite boundary). In this case the boundary does not select the structure in the bulk [17]
    • The opposite case describes the scattering of the incoming wave generated far away from the boundary with the wave vector given by an external source (or opposite boundary). In this case the boundary does not select the structure in the bulk [17].


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